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Harish-Chandra induction and restriction for finite general linear groups

Definition

Levi decompositions. Let G be a finite group and let P≤G be a subgroup that is the internal semidirect product P=L⋉U of a subgroup L≤P and a normal subgroup U⊴P with P=LU and L∩U={1} (Subgroup, Normal subgroup: invariance under conjugation); one calls P a parabolic subgroup with Levi complement L and unipotent radical U when P arises this way from the finite general linear group below. The projection π:P⟶L,π(lu):=l(l∈L,u∈U), is a surjective group homomorphism with kernel U: it is the composite of the quotient map P→P/U of The quotient group G/N and coset product (gN)(hN)=ghN with the inverse of the isomorphism L→P/U, l↦lU, which is bijective because P=LU and L∩U={1} (First isomorphism theorem for groups: G/ker⁡f≅im⁡f); hence P/U≅L.

Inflation. Let R be a commutative ring and let V be an R-linear L-module (An R-linear action of G on a left R-module, and a G-module over R). The inflation of V from L to P is the R-module V together with the P-action p⋅v:=π(p)⋅v(p∈P, v∈V), which is well defined because π is a homomorphism, and under which every element of U acts as the identity; we write Inf⁡LPV for this R-linear P-module.

Harish-Chandra induction. With V as above, the Harish-Chandra induction of V from L to G (with respect to the parabolic P) is the R-linear G-module RLG(V):=Ind⁡PG ⁣(Inf⁡LPV), the induction from P to G of The induced R-linear G-module Ind⁡HGW as H-covariant functions on G; thus RLG(V) is the set of functions f:G→V with f(gp)=π(p)−1f(g) for all g∈G, p∈P, and (x⋅f)(g)=f(x−1g).

Harish-Chandra restriction. Let X be an R-linear G-module. Its U-invariants are XU:={ x∈X:u⋅x=x for every u∈U }, an R-submodule of X that is stable under P. Define the Harish-Chandra restriction of X from G to L (with respect to P) to be XU equipped with the L-action l⋅x:=l x(l∈L, x∈XU), the restriction of the P-action. This is well defined as an action of L, and it depends only on the class of l in P/U≅L: if p∈P has π(p)=l, then p=lu with u∈U and px=lux=lx for x∈XU. We write ∗ ⁣RLG(X):=XU for this R-linear L-module.

Functoriality. If φ:V→V′ is a morphism of R-linear L-modules, then φ is also P-linear for the inflated actions, and postcomposition with φ defines a morphism RLG(φ):RLG(V)→RLG(V′) of R-linear G-modules, because (φ∘f)(gp)=π(p)−1φ(f(g)); the assignments V↦RLG(V) and X↦∗ ⁣RLG(X) are additive functors between the categories of R-linear L-modules and R-linear G-modules, and X↦XU acts on morphisms by restriction since the action of U is R-linear by An R-linear action of G on a left R-module, and a G-module over R.

The case of finite general linear groups. Now let n≥1, let q be a prime power and put G=GL⁡n(Fq), with diagonal torus T and standard flag V∙ (Standard subgroups of finite general linear groups). For a composition α of n the standard parabolic subgroup Pα has the Levi decomposition Pα=Lα⋉Uα (Compositions, partial flags, and standard parabolics, Block Levi decomposition of standard parabolics), so the constructions above apply with P=Pα, L=Lα, U=Uα; we write RLαG(V):=Ind⁡PαG ⁣(Inf⁡LαPαV),∗ ⁣RLαG(X):=XUα. More generally, a subgroup of G is a split Levi subgroup when it is of the form gLαg−1 for some g∈G and composition α, and a split parabolic subgroup is a subgroup of the form gPαg−1; such a subgroup has the Levi decomposition gPαg−1=(gLαg−1)⋉(gUαg−1), and the general construction above attaches to it the functors RLG and ∗ ⁣RLG for L=gLαg−1. For an arbitrary split parabolic the definitions therefore involve no further choice: the parabolic subgroup P and its unipotent radical U are part of the data, and the notation RLG, ∗ ⁣RLG records only the Levi. For complex modules and coordinate parabolics obtained by ordering the same coordinate blocks, the parabolic-independence theorem of this page proves that these functors depend, up to natural isomorphism, only on L. Over a general coefficient ring R, the parabolic P remains part of the functor data; when needed we display it as RLG,P and ∗ ⁣RLG,P.

Standing conventions. Except where another coefficient ring is named, all modules on this page are complex vector spaces, so R=C, the group algebras are semisimple by Maschke's theorem for finite groups over fields whose characteristic does not divide ∣G∣, and the functors above are the complex Harish-Chandra functors of Dudas–Michel. For finite-dimensional V one has dim⁡CRLG(V)=[G:P]dim⁡CV, because an induced module is free over the index of P in G (the functions of The induced R-linear G-module Ind⁡HGW as H-covariant functions on G are determined by their values on a set of left coset representatives), and dim⁡C∗ ⁣RLG(X)≤dim⁡CX.

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